EE101 Course Review Topics
Spring 2003
Units and prefixes
Charge: coulombs (C)
Current: amps (A) coulombs per second
Voltage: volts (V) energy per coulomb
Period: seconds (s)
Frequency: hertz (Hz)
Resistance: ohms ( )
Capacitance: farads (F)
106: mega (M)
103: kilo (k)
10-3: milli (m)
10-6: micro ( )
10-9: nano (n)
10-12: pico (p)
Ohm’s Law V = I R
The voltage across a resistor is equal to the current multiplied by the resistance.
Example:
You measure 100 mA flowing through a 100
across the resistor?
V = I R = (100 mA · 100
resistor. What is the voltage
) = (0.1 · 100) volts = 10 volts
Example:
What is the current in the circuit below?
The circuit has 5 volts across a 2 k
resistor, so I = (5 volts / 2 k ) = 2.5 mA
R1 = 2 k ohms
+
5 V dc
-
I
Period and Frequency
The period of a waveform is the duration of one cycle. Period is a time interval, so it is
measured in seconds.
The frequency of a waveform is the number of cycles that occur in one second (cycles per
second = hertz [Hz]).
Since the period is the duration of one cycle and frequency is the number of cycles per
second, period and frequency are reciprocals: period = 1/frequency, and
frequency = 1/period.
Nodes, Loops, and Branches
A node is a place in a circuit where two or more components come together. The node
encompasses the entire portion of the circuit wiring that comprises the node. A circuit
must have at least two nodes.
Example: 3 nodes
R1
+
5 V dc
-
R2
R3
A loop is a connected path through a sequence of elements that starts and ends at the
same node without crossing itself. A circuit must have at least one loop. If there is more
than a single loop, the separate loops of a circuit generally partially overlap one another.
Example: 3 loops
+
5 V dc
-
A branch is a path from one node to an adjacent node. A circuit branch contains one or
more components (resistors, capacitor, etc.).
Kirchhoff’s Voltage Law (KVL)
If we move from around a circuit loop, starting and ending at the same node, KVL states
that the sum of the voltages around the loop must be zero.
Example: Following arbitrary polarities for V1 and V2, a loop equation
clockwise from upper left is
-V1 + V2 + 5 = 0
+ V1
-
R1
+
5 V dc
-
R2
V2
+
Kirchhoff’s Current Law (KCL)
Since a node can neither create, store, nor destroy electric charge, the total current
entering a node must equal the total current leaving that node. Put another way, the sum
of the currents entering a node must be zero.
Voltage and Current Measurement
Voltage and current measurements have polarity: positive or negative.
The voltmeter will indicate a positive voltage if its “+” (red) input is connected to a
higher voltage than its “-“ (black) input. Voltage can be measured without having to
change the circuit.
The ammeter will indicate a positive current if the circuit causes current to flow into the
“+” (red) terminal of the meter, out the “-“ (black) terminal, and back into the circuit.
Current measurements require you to place the meter within the circuit—in series with
the circuit branch you want to measure—so the circuit must be altered to insert the meter.
Series Resistance
If two or more resistors are connected in series (end to end), the total resistance is the sum
of the individual resistances. The total series resistance is always larger than the largest
resistor in the group, since the resistances are summed.
Rseries = R1 + R2 + … + RN
Parallel Resistance
If two or more resistors are connected in parallel (side by side), the total resistance is the
reciprocal of the sum of the reciprocals.
R parallel
1
1
R1
1
R2
...
1
RN
Logic Functions
Several basic logic functions:
AND
A B OUT
0 0
0
0 1
0
1 0
0
1 1
1
OR
A B OUT
0 0
0
0 1
1
1 0
1
1 1
1
NAND
A B OUT
0 0
1
0 1
1
1 0
1
1 1
0
NOR
A B OUT
0 0
1
0 1
0
1 0
0
1 1
0
NOT
A OUT
0
1
1
0
Voltage Gain
The voltage gain of an amplifier is the ratio of the output voltage to the input voltage.
Example:
Output voltage 3 V peak-to-peak
Input voltage 1 V peak-to-peak
Voltage gain = Vo/Vin = 3
Capacitors and time constant
A capacitor is a charge storage element. It takes time for the capacitor to charge up, and
the charging time depends on the amount of current in the capacitor: small current means
a slow charge time, while a large current means a quicker charge time.
The charging time for a capacitor is often expressed in terms of a time constant given by
R · C (resistance times capacitance). The RC time constant is proportional to the time
required to charge the capacitor from zero to the applied voltage.
Diodes
A diode allows current to pass in one direction, but blocks current in the other direction.
Semiconductor diodes show a forward voltage of 0.5 – 1.0 volt when current passes in
the forward direction. Essentially no current passes in the reverse direction.
Lab instruments
Digital multimeter (DMM): measures voltage, current, or resistance.
Function generator (or signal generator): produces alternating voltage signals (such as
sine waves) with a particular frequency and amplitude.
DC power supply (or bench supply): produces a constant voltage like a battery, except
derived electronically from the 120V line voltage.
Oscilloscope: displays voltage vs. time for measurement of signal amplitude, period, and
relative phase.